A beam of unpolarized light passes through a tourmaline crystal A and then it passes through a second tourmaline crystal B oriented so that its principal plane is parallel to that of A. The intensity of emergent light is $I_0$. Now B is rotated by $45^\circ$ about the ray. The emergent light will have intensity $(\cos 45^\circ = \frac{1}{\sqrt{2)$
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Logic Tip: Malus's Law ($I = I_{max} \cos^2 \theta$) creates a very predictable pattern:
At $0^\circ \rightarrow I_{max}$
At $45^\circ \rightarrow I_{max}/2$
At $60^\circ \rightarrow I_{max}/4$
At $90^\circ \rightarrow 0$ (crossed polarizers).